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1.
为了解决现有的基于量子点荧光共振能量转移体系的生物毒性问题,选用无毒的ZnS∶Cu量子点与罗丹明B构建新型荧光共振能量转移体系。通过共沉淀法成功制备了形貌均一的ZnS∶Cu纳米晶量子点。在此基础上,测试了不同掺杂浓度的ZnS∶Cu量子点及罗丹明B的荧光光谱。然后,通过对ZnS∶Cu量子点的表面修饰构建了以ZnS∶Cu量子点为供体、罗丹明B为受体的荧光共振能量转移体系。实验结果表明:ZnS∶2%Cu量子点的发光光谱与罗丹明B的吸收光谱在481 nm处有较大重合,说明构建荧光共振能量转移的最佳铜掺杂摩尔分数为2%。通过计算发现以ZnS∶2%Cu量子点为供体、罗丹明B为受体的荧光共振能量转移体系的能量转移效率为25.8%。进一步实验结果表明,罗丹明B浓度也能够影响能量转移。  相似文献   

2.
何志聪  李芳  李牧野  魏来 《物理学报》2015,64(4):46802-046802
以波长为780 nm、重复频率为76 MHz、脉宽为130 fs的飞秒激光作为激发光源, 采用超快时间分辨光谱技术研究了CdTe量子点-铜酞菁复合体系的荧光共振能量转移. 实验结果表明, 在780 nm的双光子激发条件下, 复合体系中CdTe量子点的荧光寿命随着铜酞菁溶液浓度的增加而减少, 荧光共振能量转移效率增加. 同时也研究了激发功率对荧光共振能量转移效率的影响. 结果表明, 随着激发光功率的增加, 复合体系溶液中CdTe量子点的荧光寿命增加, 荧光共振能量转移效率减小, 其物理机理是因为高激发功率下的热效应和由双光子诱导的高阶激发态的跃迁. 当激发光功率为200 mW时, 双光子荧光共振能量转移效率为43.8%. 研究表明CdTe量子点-铜酞菁复合体系是非常有潜力的第三代光敏剂.  相似文献   

3.
以巯基乙酸为稳定剂合成了CdTe量子点,并利用其与牛血清白蛋白(BSA)组成了荧光共振能量转移体系,考察BSA(供体)和CdTe量子点(受体)之间的荧光共振能量转移的最佳条件,建立了荧光共振能量转移增敏法测定Zn2+的新方法.在pH 7.4的Tris-HCl缓冲溶液中,Zn2+能对能量转移体系中CdTe量子点增敏从而测定锌的含量.Zn2+浓度在0.49-4.88μg/mL浓度范围内与CdTe量子点荧光强度呈现良好线性关系(r=0.9996),检出限为0.13μg/mL,RSD为3.2%,平均回收率为99.5%(n=5).方法适用于果汁饮料中微量锌的测定.  相似文献   

4.
李牧野  李芳  魏来  何志聪  张俊佩  韩俊波  陆培祥 《物理学报》2015,64(10):108201-108201
采用时间分辨荧光光谱技术研究了在双光子激发下不同尺寸的量子点与罗丹明B 之间的荧光共振能量转移. 研究结果表明, 在800 nm的双光子激发条件下, 体系间能量转移效率随着供体吸收光谱与受体荧光光谱的光谱重叠程度增加而增加; 理论分析表明, 供体和受体间的Förster半径增加是导致其双光子能量转移效率增大的物理原因. 同时, 研究了罗丹明B浓度对荧光共振能量转移效率的影响. 研究结果表明, 量子点的荧光寿命随着罗丹明B浓度的增加而减小; 量子点与罗丹明B之间的荧光共振能量转移效率随着罗丹明B浓度的增加而增加; 当罗丹明B浓度为3.0×10-5 mol·L-1时, 双光子荧光共振能量转移效率为40.1%.  相似文献   

5.
刘义章  孙军勇  王磊  周凯  巩振虎 《发光学报》2017,38(10):1353-1358
基于半导体聚合物量子点和亚甲基蓝间的荧光共振能量转移构筑了一种铋离子荧光探针。亚甲蓝通过静电作用吸附到半导体聚合物量子点表面使其荧光发生猝灭。铋离子存在时,由于它与半导体聚合物量子点的结合力强于亚甲蓝,使体系的能量转移得到抑制,荧光恢复。在最优化条件下,线性范围为0~0.5%mol/L(R=0.995 5),最低检出限为16 nmol/L。该方法成功用于湖水中的Bi3+测定,结果令人满意。  相似文献   

6.
研究CdTe量子点(供体)和罗丹明B(受体)之间荧光共振能量转移的最佳条件,建立了荧光共振能量转移猝灭法测定金银花中微量铜的新方法.采用十六烷基三甲基溴化铵,在pH 6.00的Tris-HCl缓冲液中,Cu2+能对能量转移体系中罗丹明B荧光峰强猝灭从而测定铜的含量.Cu2+浓度在1.3×10-4~3.1×10-2 μg...  相似文献   

7.
微腔中单分子对荧光共振能量转移光谱学的理论研究   总被引:1,自引:1,他引:0  
生物大分子动态的结构变化能够使用单分子对荧光共振能量转移谱技术来研究.主要研究了微腔在单分子对共振能量转移实验中有效提高相应单分子对的荧光发射信号的作用,从而提高该技术的时间分辨率.研究发现.由于受体一微腔的强耦合相互作用,光学微腔使得受体分子变成了一个类似于单原子激光的激光体.此外,随着距离的增加.受体的光子数会很快下降.微腔使受体的发射光对单分子对间的距离有更大的依赖性,在腔体中进行单分子对共振能量转移实验町以得到更高的时间分辨率.研究结果为单分子对荧光共振能量转移技术提供了实验方法和理论指导.  相似文献   

8.
利用巯基丙酸包覆的In P@Zn S量子点(QDs)与Dured构建了一种检测DNA的荧光探针。在该探针中,以环境友好型带负电的In P@Zn S量子点为荧光团,与带正电的Dured通过静电结合,构建了In P@Zn S QDs/Dured纳米荧光探针。通过荧光共振能量转移(FRET)机理,量子点荧光被猝灭;当DNA存在时,Dured与DNA的特异性结合使Dured从In P@Zn S QDs表面脱附,FRET过程被打断,In P@Zn S QDs荧光恢复,以荧光"关-开"方式检测DNA。该探针检测DNA的线性范围为2.0~275.0 ng·L-1,检测限为1.0 ng·L-1,并可用于模拟生物生理条件下的DNA检测。  相似文献   

9.
当量子点粒度分布为高斯分布时,应用有效质量近似,在低浓度掺杂范围内,得到了量子点荧光辐射谱线形函数与量子点尺寸之间的一般关系,解释了尺寸涨落对线形展宽的影响。对II-VI族的Cd Se量子点和IV-VI族的Pb Se量子点的数值计算表明:量子点荧光谱线的半峰全宽、荧光辐射强度、峰值波长等与实验结果基本一致。量子点尺寸的粒度分布对荧光辐射谱线展宽有较大的影响。荧光辐射谱展宽是一种非均匀展宽。  相似文献   

10.
开发了CdS量子点用于牛血清白蛋白(BSA)表面压印的方法,将CdS量子点掺杂进BSA的分子压印聚合物中. 实验过程中对制备条件和吸附条件进行了优化. 量子点(QDs)和量子点分子压印聚合物(QDs-MIP)的形貌用扫描电子显微镜进行了表征. 当该QDs-MIP重新结合模板分子BSA时,CdS量子点的荧光被淬灭. 荧光淬灭的原因可能是量子点与模板蛋白质分子之间的荧光共振能量转移. 该聚合物对压印分子的吸附为单分子层吸附,符合Langmuir等温吸附模型. 化学吸附为速率控制步骤. 该新型聚合物的最大吸附容量可达226.0 mg/g,比未掺杂量子点的BSA压印聚合物提高142.4 mg/g.  相似文献   

11.
Two-dimensional scanning of a 0.6328 mum guided-light beam has been realized using noncolinear acousto-optic (AO) coplanar Bragg diffraction together with colinear AO guided-mode to substrate radiation-mode conversion in a Z-cut Xpropagation LiNbO3 proton-exchanged (PE) waveguide. The two surface acoustic (SAW) waves utilized are at the center frequencies of 500 and 200 MHz, propagating in the Y and X axes, respectively. Two-dimensional scanning of approximately 720 resolvable light beam spots, namely, 18 40 (horizontal vertical) scanning, has been demonstrated using a light beam of 1.0 mm aperture. The total number of resolvable beam spots can be greatly increased from 720 by simply utilizing SAW transducers of larger bandwidth and a light beam of greater aperture. It should also be possible to significantly increase the diffraction efficiency from 3 % by optimizing the parameters of the PE waveguide and the SAWs.  相似文献   

12.
A review of schemes for multiple access in fiber optic networks shows that a hybrid of wavelength and code division multiple access (WCDMA) combines the best features of both. In particular, the hybrid scheme retains the large information carrying capacity of wavelength division multiple access (WDMA) and flexibility of code division multiple access (CDMA). In this paper WDMA, optical CDMA (OCDMA), and WCDMA networks are discussed. In OCDMA networks, concept of incoherent and coherent coding including inverse decoding and matched filter is introduced. The delay performance of both WDMA and WCDMA networks, under the simple suboptimum access protocols based on cyclic search, is computed. It has been shown quantitatively that tuning delay significantly affects the delay performance of both WDMA and WCDMA networks. Futhermore, delay performance of WCDMA networks is always better than the WDMA networks for the same tuning delay, load, and number of users.  相似文献   

13.
Results of a study of the effect of γ-radiation on the spectral luminescence properties of cadmium tungstate crystals doped with silver, bismuth, and molybdenum cations are presented. Spectral characteristics of the nondnnnoped crystals are briefly described. Absorption and photo and X-ray luminescence spectra of the crystals taken before and after exposure to γ-radiation (5.5·104 Gy) are compared. It is found that the spectral characteristics of the crystals doped with silver, bismuth, and molybdenum cations do not change markedly after the exposure. The relation between the type of impurity-induced defects, individual characteristics of the impurity cations, and the character of the effect of γ-radiation on the spectral luminescence properties of impure crystals is analyzed (preliminarily). Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 64, No. 1, pp. 55–60, January–February, 1997.  相似文献   

14.
A simple technique of pulse compression, based on the linear chirp compensation of self-phase modulation (SPM) spectra in dispersion shifted fibers, is demonstrated. The optimization procedure is carried out, for a short span of a single-mode fiber, using a parabolic law, which describes the behavior of the squared output pulse width versus the pump peak power in the case of Gaussian pulses. The experimental results give a minimum pulse duration of 233 fs, which is in good agreement with the model. Shorter and coherent pulses, down to 90 fs, have been obtained by inserting an interference filter at the optical output.  相似文献   

15.
The Shanghai Synchrotron Radiation Facility(SSRF)booster ring,a full energy injector for the storage ring,is deigned to accelerate the electron beam energy from 150MeV to 3.5GeV that demands high extraction efficiency at the extraction energy with low beam loss rate when electrons are ramping.Closed orbit distortion(COD)caused by bending magnet field uniformity errors which affects the machine performance harmfully could be effectively reduced by bending magnet location sorting.Considering the affections of random errors in measurement,both ideal sorting and realistic sorting are studied based on measured bending magnet field uniformity errors and one reasonable combination of bending magnets which can reduce the horizontal COD by a factor of 5is given as the final installation sequence of the booster bending magnets in this paper.  相似文献   

16.
17.
We measure the waveform and phase curves of short optical pulses before and after transmission over different lengths of fibers by use of the pulse analyzer with the frequency-resolved optical gating (FROG),and numerically simulate pulse evolution under the experimental conditions.The nonlinear coefficient of the fiber is given by comparing the experimental results with the numerical ones.Difference between the experiment and numerical simulation is analyzed.  相似文献   

18.
Resonance scattering of elastic spherical shell and cylindrical shell while the surrounding fluid medium has absorption is studied. The normal mode solution derived using exact elastic theory and the separation of variables is still applicable. However, the scattering form function has to be modified for the absorbing medium, otherwise the unreasonable result would be obtained. The backscattering form function in the absorbing medium is redefined, and the form function of elastic spherical and cylindrical shell with vacuum or solid matter filled is calculated in various absorption conditions. The results show that the absorption of surrounding fluid leads to notable attenuation of the coincidence resonances in the mid-frequency, but it has a little influence on the low-frequency resonance scattering induced by the filler inside the shell.  相似文献   

19.
A versatile and low-cost single-beam self-referenced phase-sensitive surface plasmon resonance(SPR)sensing system with ultra-high resolution performance is presented.The system exhibits a root-mean-square phase fluctuation of ±0.0028.over a period of 45 min.i.e.a resolution of±5.2×10-9 refractive index units.The enhanced performance has been achieved through the incorporation of three design elements:a true single-beam configuration enabling complete self-referencing so that only the phase change associated with SPR gets detected,a differential measurement scheme to eliminate spurious signals not related to the sensor response,and the elimination of retardation drifts by incorporating temperature stabilization in the liquid crystal phase modulato .Our design should bring the detection sensitivity of non-labeling SPR biosensing closer to that achievable by conventional fluorescence-based techniques.  相似文献   

20.
Ta2O5 films are prepared on BK7 substrates with conventional electron beam evaporation deposition.The effects of SiO2 protective layers and annealing on the laser-induced damage threshold (LIDT) of the films are investigated.The results show that SiO2 protective layers exert little influence on the electric field intensity(EFI)distribution,microstructure and microdefect density but increase the absorption slightly.Annealing iS effective on decreasing the microdefect density and the absorption of the films.Both SiO2 protective layers and annealing are beneficial to the damage resistance of the films and the latter is more effective to improve the LIDT.Moreover,the maximal LIDT of Ta2O5 films is achieved by the combination of SiO2 protective layers and annealing.  相似文献   

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